Page 98 - Curvature and Homology
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80         11.  TOPOLOGY  OF  DIFFERENTIABLE  MANIFOLDS

         7.  Define themapp:AP(V*)-tAn-P(V*)  by  p=hoy,  wherey:  AP(V*)
         +    (V)  is the  natural identification map  determined by  the inner product
         in  AP(V*).  Then, p is the star operation of  Hodge.
         8.  Let  V be a vector space (over R) with the properties:
          (i)  V is the direct sum of  subspaces Vp  where p runs through non-negative
         integers and
           (ii)  V has a coboudary operator that is an endomorphism d of  V such that
         d,Vv  C V9+l with  d,,,d,   = 0  where  d,  denotes the  restriction  of  d  to  Vr.
         The vector space
                                       kernel d,
                               Hp(V) =
                                       image d,,
         is called the p*  cohomology vector  space (or group) of  V.  A theory based on  V
         together with the operator d is usually called a cohomology theory or d-cohomology
         theory  when emphasis on  the  coboundary operator  is required.  We have seen
         that the Grassman algebra A(T*) with the exterior differential operator d gives
         rise  to  the  de Rharn cohomology theory.  On  the other hand, a  cohomology
         theory is defined by the pair  (A(T*),6)  on  a  Riemannian manifold by setting
         A-9  = A 9, p = 0,1,2, *-* . Prove that the * operator induces an isomorphism
         between the two cohomology theories.


         B.  The operators H and G on a compact manifold
         1.  Show that for any a E AP(T*) there exists a unique p-form H[a] in A UT*)
         with  the property (a#)  = (H[or],/3) for all /3 E A  T*).
         2.  Prove that H[H[u]]  = H[a] for anyp-form a.
         3.  For  a  given p-form  a  there  exists  a p-form  /3  satisfying  the  differential
         equation A/3 = a - H[a].  Show that  any  two  solutions differ  by  a harmonic
         p-form  and thereby establish the existence of  a unique solution orthogonal to
         A&(T*). Denote this solution by Ga and show that it is charaderized by the
         conditions
                         a = AGa + H[a]  and  (Ga,/3) = 0
         for any   E AHT*).
           The operator G is called the Green's operator.
         4.  Prove that H[Ga]  vanishes for any p-form  a.
         5.  Prove:
           (a) The operators H and G commute with d,  6, A  and *;
           (b) G is sey-dud, that is
                                 (Ga,B) = (a,G/3)
         for any a, /3 of  degree P;
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